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This is the optical power loss measured between a WDM channel input and output ports, see Figs 619a and 620 The measurement unit is dB Maximum insertion loss for any WDM channel is provided in specifications The maximum insertion loss may differ for DWDM multiplexer and demultiplexer units Maximum insertion loss for FBG and TFF WDMs can also be specified for a mux/demux matched pair This is the total loss for both multiplexer and demultiplexer units in the fiber link Internally the optical WDM signals propagate from one channel filter to the other in a sort of series fashion, see Figs 64 and 66 The signal that matches the channel s wavelength is dropped or else it continues to the next channel filter Hence, filters closer to the aggregate (common) fiber end have a lower insertion loss than filters further from it Filter channels in matched multiplexer and demultiplexer pairs are sequenced in opposite directions from aggregate fiber such that the combined loss for each channel is more uniform and less than the combined loss of the two highest loss channels This method provides a lower maximum insertion loss for the pair For OADMs, the insertion loss is divided into through loss and channel add/drop loss The OADM through loss is measured between the two common ports The OADM channel add/drop loss is measured from the common port and a drop port, see Fig 619b

0 20 40 60 80 100 120140160180 MIX INDEX PERCENT (C+3D)

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where BWE = photodiode s maximum 3 dB bandwidth, Hz CT = total photodiode s capacitance, F RL = load resistance, There is a trade-off when selecting an appropriate load resistance Increasing the load resistance increases the input voltage to the amplifier and therefore the output It also reduces thermal noise and improves sensitivity However, a larger load resistance decreases the signal bandwidth and dynamic range, see Eq (1016) PIN Photodiodes are available with very high bandwidths that are well over 10 Gbps, however APD photodiodes are currently only available up to 10 Gbps Other major components in a receiver are the photo current amplifier, noise filter, and decision circuit, see Fig 107 The receiver converts the optical signal to a conditioned electrical digital signal in the following sequence First the photodiode converts the fiber optical signal to an electrical current signal Then the pre-amp amplifies the signal voltage across the load resister RL It also incorporates automatic gain control circuitry (AGC) that helps to keep the output signal voltage stable and increases the receiver s dynamic range Next the low pass noise filter removes unwanted high frequency noise components and improves the signal to noise ratio (SNR) This is because noise is directly dependent on electrical bandwidth The wider the bandwidth, the more noise power is allowed into the circuit and therefore the lower the SNR The bandwidth needs to be just wide enough to pass all the signal The rule of thumb is that the receiver s electrical bandwidth should be approximately 07 times the bit rate, see Eq (1017) For example, for a 10 Gbps signal the bandwidth should be 7 GHz BWE = 0 7 R where BWE = electrical bandwidth, Hz R = transmission rate, bps (1017)

0 20 40 60 80 100 120140160180 MIX INDEX PERCENT (C+3D)

The output shaft of the servomotor is now free to rotate continuously A pulse width of 1 ms sent 50 to 60 times per second (Hz) will cause the servo motor to rotate in one direction A pulse width of 2 ms will cause the servo motor to turn in the opposite direction There are two ways we can stop the servomotor from rotating The first method is to simply stop sending pulses to the servomotor The second method is a little trickier A pulse width of approximately 15 ms will stop the servo

0 20 40 60 80 100 120140160180 MIX INDEX PERCENT (C+3D)

Finally the decision circuitry determines the logical meaning of the voltage value in a time slot and reproduces the original signal If the voltage value is above the decision threshold a logical one is assigned to the time slot and if it is below the decision threshold a logical zero is assigned to the threshold, see Fig 315 Noise is generated in the front end of the receiver (photodiode to the decision circuitry) that degrades signal performance and decreases the SNR The two main sources of receiver noise are shot noise and thermal noise Shot noise occurs in the photodiode and is due to the random distribution of electrons generated by the photo detection process Thermal noise occurs in any component and is due to random electron motion due to temperature Thermal noise decreases when the component s temperature is lowered and is nonexistent at absolute zero The photodiode, load resistor, and pre-amp all contribute to receiver thermal noise Total noise generated by the receiver is equal to the sum of all receiver noise variances The noise generated for the two-signal logical level one and zero, is different Total generated noise for each logic level is shown in Eqs (1018) and (1019)

FIGURE 12-15

Arrival and departure delay indices for Example Problem 12-8

(1018)

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